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C 477.3
XVIII. Catalogue of 500 new Nebula, nebulous Stars, planetary
Nebula, and Clusters of Stars ; with Remarks on the Con-
struction of the Heavens. By William Herschel, LL. D.
F. R. S.
Read July 1, 1802.
oince the publication of my former two catalogues of nebulse,
I have, in the continuation of my telescopic sweeps, met with a
number of objects that will enrich our natural history, as it
may be called, of the heavens. A catalogue of them will be
found at the end of this paper, containing 500 new nebulae,
nebulous stars, planetary nebulse, and clusters of stars. These
objects have been arranged in eight classes, in conformity
with the former catalogues, of which the present one is there-
fore a regular continuation. This renders it unnecessary to give
any further explanation, either of the contents of its columns, or
the abbreviations which have been used in the description of
the objects.
It has hitherto been the chief employment of the physical
astronomer, to search for new celestial objects, whatsoever might
be their nature or condition ; but our stock of materials is now
so increased, that we should begin to arrange them more scien-
tifically. The classification adopted in my catalogues, is little
more than an arrangement of the objects for the convenience
of the observer, and may be compared to the disposition of the
books in a library, where the different sizes of the volumes is
mdcccii. 3 Q
478 Tk. Herschel's Catalogue
often more considered than their contents. But here, in dividing
the different parts of which the sidereal heavens are composed
into proper classes, I shall have to examine the nature of the
various celestial objects that have been hitherto discovered, in
order to arrange them in a manner most conformable to their
construction. This will bring on some extensive considerations,
which would be too long for the compass of a single paper; I
shall therefore now only give an enumeration of the species
that offer themselves already to our view, and leave a particular
examination of the separate divisions, for some early future
occasions.
In proceeding from the most simple to the more complex
arrangements, several methods, taken from the known laws of
gravitation, will be suggested, by which the various systems
under consideration may be maintained ; but here also we shall
confine ourselves to a general review of the subject, as obser-
vation must furnish us first with the necessary data, to establish
the application of any one of these methods on a proper
foundation.
ENUMERATION OF THE PARTS THAT ENTER INTO THE CONSTRUC-
TION OF THE HEAVENS.
I. Of insulated Stars.
In beginning our proposed enumeration, it might be expected
that the solar system would stand foremost in the list ; whereas,
by treating of insulated stars, we seem, as it were, to overlook one
of the great component parts of the universe. It will, however,
soon appear that this very system, magnificent as it is, can only
rank as a single individual belonging to the species which we
are going to consider.
of 500 nevo Nebula, and Clusters of Stars. 479
By calling a star insulated, I do not mean to denote its being
totally unconnected with all other stars or systems ; for no one,
by the laws of gravitation, can be intirely free from the in-
fluence of other celestial bodies. But, when stars are situated at
such immense distances from each other as our sun, Arcturus,
Capella, Lyra, Sirius, Ganobus, Markab, Bellatrix, Menkar,
Shedir, Algorah, Propus, and numberless others probably are,
we may then look upon them as sufficiently out of the reach of
mutual attractions, to deserve the name of insulated stars.
In order not to take this assertion for granted, without some
examination, let us admit, as is highly probable, that the whole
orbit of the earth's annual motion does not subtend more than
an angle of one second of a degree, when seen from Sirius. In
consequence of this, it appears by computation, that our sun and
Sirius, if we suppose their masses to be equal, would not fall
together in less than 33 millions of years, even though they
were not impeded by many contrary attractions of other neigh-
bouring insulated stars; and that, consequently, with the
assistance of the opposite energies exerted by such surrounding
stars, these two bodies may remain for millions of ages, in a
state almost equal to undisturbed rest. A star thus situated may
certainly deserve to be called insulated, since it does not imme-
diately enter into connection with any neighbouring star; and
it is therefore highly probable, that our sun is one of a great
number that are in similar circumstances. To this may be
added, that the stars we consider as insulated are also sur-
rounded by a magnificent collection of innumerable stars, called
the milky-way, which must occasion a very powerful balance
of opposite attractions, to hold the intermediate stars in a state
of rest. For, though our sun, and all the stars we see, may
3Q a
480 Dr. Herschel's Catalogue
truly be said to be in the plane of the milky- way, yet I am now
convinced, by a long inspection and continued examination of
it, that the milky-way itself consists of stars very differently
scattered from those which are immediately about us. But of
this, more will be said on another occasion.
From the detached situation of insulated stars, it appears that
they are capable of being the centres of extensive planetary
systems. Of this we have a convincing proof in our sun, which,
according to our classification, is one of these stars. Now, as
we enjoy the advantage of being able to view the solar system
in all its parts, by means of our telescopes, and are therefore
sufficiently acquainted with it, there will be no occasion to enter
into a detail of its construction.
The question will now arise, whether every insulated star be
a sun like ours, attended with planets, satellites, and numerous
comets ? And here, as nothing appears against the supposition,
we may from analogy admit the probability of it. But, were we
to extend this argument to other sidereal constructions, or, still
farther, to every star of the heavens, as has been done fre-
quently, I should not only hesitate, but even think that, from
what will be said of stars which enter into complicated sidereal
systems, the contrary is far more likely to be the case ; and that,
probably, we can only look for solar systems among insulated
stars.
II. Of Binary sidereal Systems, or double Stars.
The next part in the construction of the heavens, that offers
itself to our consideration, is the union of two stars, that are
formed together into one system, by the laws of attraction.
If a certain star should be situated at any, perhaps immense,
of 500 new Nebula, and Clusters of Stars. 481
distance behind another, and but very little deviating from the
line in which we see the first, we should then have the ap-
pearance of a double star. But these stars, being totally uncon-
nected, would not form a binary system. If, on the contrary,
two stars should really be situated very near each other, and at
the same time so far insulated as not to be materially affected
by the attractions of neighbouring stars, they will then compose
a separate system, and remain united by the bond of their own
mutual gravitation towards each other. This should be called a
real double star; and any two stars that are thus mutually
connected, form the binary sidereal system which we are now
to consider.
It is easy to prove, from the doctrine of gravitation, that two
stars may be so connected together as to perform circles, or
similar ellipses, round their common centre of gravity. In this
case, they will always move in directions opposite and parallel
to each other ; and their system, if not destroyed by some foreign
cause, will remain permanent.
Figure 1 (Plate XVI.) represents two equal stars a and b,
moving in one common circular orbit round the centre 0, but
in the opposite directions of at and bt. In Fig. 2 we have a
similar connection of the two stars a b; but, as they are of dif-
ferent magnitudes, or contain unequal quantities of matter, they
will move in circular orbits of different dimensions round their
common centre of gravity 0. Fig. 3 represents equal, and Fig. 4,
unequal stars, moving in similar elliptical orbits round a com-
mon centre ; and, in all these cases, the directions of the tangents
1 1, in the places a b, where the stars are, will be opposite and
parallel, as will be more fully explained hereafter.
These four orbits, simple as they are, open an extensive field
48s Dr. Herschel's Catalogue
for reflection, and, I may add, for calculation. They shew, even
before we come to more complicated combinations, where the
same will be confirmed, that there is an essential difference
between the construction of solar and sidereal systems. In
each solar system, we have a very ponderous attractive centre,
by which all the planets, satellites, and comets are governed,
and kept in their orbits. Sidereal systems take a greater scope :
the stars of which they are composed move round an empty
centre, to which they are nevertheless as firmly bound as the
planets to their massy one. It is however not necessary here to
enlarge on distinctions which will hereafter be strongly sup-
ported by facts, when clusters of stars come to be considered.
I shall only add, that in the subordinate bodies of the solar
system itself, we have already instances, in miniature, as it may
be called, of the principle whereby the laws of attraction are
applicable to the solution of the most complicated phenomena
of the heavens, by means of revolutions round empty centres.
For, although both the earth and its moon are retained in their
orbits by the sun, yet their mutual subordinate system is such,
that they perform secondary monthly revolutions round a centre
without a body placed in it. The same indeed, though under
very narrow limits, may be said of the sun and each planet
itself.
That no insulated stars, of nearly an equal size and distance,
can appear double to us, may be proved thus. Let Arcturus and
Lyra be the stars : these, by the rule of insulation, which we
must now suppose can only take place when their distance from
each other is not less than that of Sirius from us, if very accu-
rately placed, would be seen under an angle of 60 degrees from
each other. They really are at about 59 . Now, in order to
of 500 new Nebula,, and Clusters of Stars. 483
make these stars appear to us near enough to come under the
denomination of a double star of the first class, we should re-
move the earth from them at least 41353 times farther than
Sirius is from us. But the space-penetrating power of a 7-feet
reflector, by which my observations on double stars have been
made, cannot intitle us to see stars at such an immense distance ;
for, even the 40-feet telescope, as has been shewn,* can only
reach stars of the 1343d magnitude. It follows, therefore, that
these stars could not remain visible in a 7-feet reflector, if they
were so far removed as to make their angular distance less than
about 24^ minutes ; nor could even the 40-feet telescope, under the
same circumstances of removal, shew them, unless they were to
be seen at least sf- minutes asunder. Moreover, this calculation
is made on a supposition that the stars of which a double star is
composed, might be as small as any that can possibly be per-
ceived ; but if, on the contrary, they should still appear of a
considerable size, it will then be so much the more evident that
such stars cannot have any great real distance, and that, con-
sequently, insulated stars cannot appear double, if they are situ-
ated at equal distances from us. If, however, their arrangement
should be such as has been mentioned before, then, one of them
being far behind the other, an apparent double star may cer-
tainly be produced ; but here the appearance of proximity
would be deceptive ; and the object so circumstanced could not
be classed in the list of binary systems. However, as we must
grant, that in particular situations stars apparently double may
be composed of such as are insulated, it cannot be improper to
consult calculation', in order to see whether it be likely that the
700 double stars I have given in two catalogues, as well as
* See Phil. Trans, for 1800, Part I. page 83.
484 T>r. Herschel's Catalogue
many more I have since collected, should be of that kind. Such
an inquiry, though not very material to our present purpose,
will hereafter be of use to us, when we come to consider more
complicated systems. For, if it can be shown that the odds are
very much against the casual production of double stars, the
same argument will be still more forcible, when applied to treble,
quadruple, or multiple compositions.
Let us take £" Aquarii, for an instance of computation. This
star is admitted, by Flamsteed, De la Caille, Bradley, and
Mayer, to be of the 4th magnitude. The two stars that com-
pose it being equal in brightness, each of them may be supposed
to shine with half the light of the whole lustre. This, according
to our way of reckoning magnitudes,* would make them 4m
x y/a = 5fm ; that is, of between the 6th and 5th magnitude
each. Now, the light we receive from a star being as the square
of its diameter directly, and as the square of its distance in-
versely, if one of the stars of £ Aquarii be farther off than the
stars of between the 6th and 5th magnitude are from us, it must
be so much larger in diameter, in order to give us an equal
quantity of light. Let it be at the distance of the stars of the
7th magnitude; then its diameter will be to the diameter of
the star which is nearest to us as 7 to 5^, and its bulk as 1,885
to 1 ; which is almost double that of the nearest star. Then,
putting the number of stars we call of between the 6th and
5th magnitude at 450, we shall have 686 of the 7th magnitude
to combine with them, so that they may make up a double star
of the first class, that is to say, that the two stars may not be
more than 5" asunder. The surface of the globe contains
• The expressions 2m, 3m, 4m, &c. stand for stars at the distance of 2, 3, 4, &c.
times that of Sirius, supposed unity.
of 500 new Nebula, and Clusters of Stars. 485
34036131547 circular spaces, each of 5" in diameter; so that
each of the 686 stars will have 49615357 of these circles in
which it might be placed ; but, of all that number, a single one
would only be the proper situation in which it could make up a
double star with one of the 450 given stars. But these odds,
which are above 75! millions to one against the composition of
g Aquarii, are extremely increased by our foregoing calculation
of the required size of the star, which must contain nearly
double the mass allotted to other stars of the 7th magnitude;
of which, therefore, none but this one can be proper for making
up the required double star. If the stars of the 8th and 9th
magnitudes, of which there will be 896 and 1134, should be
taken in, by way of increasing the chance in favour of the sup-
posed composition of our double star, the advantage intended to
be obtained by the addition of numbers, will be completely
counteracted by the requisite uncommon bulk of the star which
is to serve the purpose; for, one of the 8th magnitude, ought
to be more than sf times bigger than the rest; and, if the
composition were made by a star of the 9th magnitude, no less
than four times the bulk of the other star which is to enter the
composition of the double star would answer the purpose of its
required brightness. Hence therefore it is evident, that casual
situations will not account for the multiplied phenomena of
double stars, and that consequently their existence must be
owing to the influence of some general law of nature ; now, as
the mutual gravitation of bodies towards each other is quite suf-
ficient to account for the union of two stars, we are authorised
to ascribe such combinations to that principle,
It will not be necessary to insist any further on arguments
drawn from calculation, as I shall soon communicate a series of
mdcccii. 3 R
4§S Br. Herschei/s Catalogue
observations made on double stars, whereby it will be seen, that
many of them have actually changed their situation with regard to
each other, in a progressive course, denoting a periodical revo-
lution round each other; and that the motion of some of them is
direct, while that of others is retrograde. Should these observa-*
tions be found sufficiently conclusive, we may already have their
periodical times near enough to calculate, within a certain de-
gree of approximation, the parallax and mutual distance of the
stars which compose these systems, by measuring their orbits,
which subtend a visible angle.
Before we leave the subject of binary systems, I should
remark, that it evidently appears, that our sun does not enter
into a combination with any other star, so as to form one of
these systems with it. This could not take place without our
immediately perceiving it; and, though we may have good
reason to believe that our system is not perfectly at rest, yet the
causes of its proper motion are more probably to be ascribed to
some perturbations arising from the proper motion of neigh-
bouring stars or systems, than to be placed to the account of a
periodical revolution round some imaginary distant centre.
III. Of more complicated sidereal Systems, or treble, quadruple,
quintuple, and multiple Stars.
Those who have admitted our arguments for the existence of
real double stars, will easily advance a step farther, and allow
that three stars may be connected in one mutual system of re-
ciprocal attraction. And, as we have from theory pointed out,
in figures 1, 2, 3, and 4, how two stars may be maintained
in a binary system, we shall here shew that three stars may
of soo new Nebula, and Clusters of Stars. 487
likewise be preserved in a permanent connection, by revolving
in proper orbits about a common centre of motion.
In all cases where stars are supposed to move round an empty
centre, in equal periodical times, it may be proved that an ima-
ginary attractive force may be supposed to be lodged in that
centre, which increases in a direct ratio of the distances. For
since, in different circles, by the law of centripetal forces, the
squares of the periodical times are as the radii divided by the
central attractive forces, it follows, that When these periodical
times are equal, the forces will be as the radii. Hence we con-
clude, that in any system of bodies, where the attractive forces
Of all the rest upon any one of them, when reduced to a direc-
tion as coming from the empty centre, can be shewn to be in a
direct ratio of the distance of that body from the centre, the
system may revolve together without perturbation, and remain
permanently connected without a central body.
Hence may be proved, as has been mentioned before, that
two stars will move round a hypothetical centre of attraction.
For, let it be supposed that the empty centre 0, in Fig. 1 and 3,
is possessed of an attractive force, increasing in the direct ratio
of the distances oa : ob. Then, since here ao and bo are equal,
the hypothetical attractions will be equal, and the bodies will
revolve in equal times. That this agrees with the general law
of attraction, is proved thus. The real attraction of b upon a is
-"!»-; and that of a upon' b is '-— -; and, since 6 = a, it will be
-~ : ■—- : : ao\bo ; which was required.
In Figures 2 and 4, when the stars a and b are unequal, and
their distances from also unequal, let oa = n, and ob — m;
and let the mass of matter in a=zm, and in b = ». Then the
3 R a
488 Dr. Herschel's Catalogue
attraction of b on a = —rr, will be to the attraction of a on b
= — gr, as » : w ; which is again directly as ao : bo.
I proceed now to explain a combination of three bodies,
moving round a centre of hypothetical attraction. Fig. 5 con-
tains a single orbit, wherein three equal bodies a b c, placed at
equal distances, may revolve permanently. For, the real attrac-
tion of b on a will be expressed by -~ ; but this, reduced to the
direction ao, will be only ~~ ; for, the attraction in the direc-
tion ba is to that in the direction by, parallel to ao, as -^ to
—~ -. The attraction also of c on a is equal to that of b on a ;
therefore the whole attraction on a, in a direction towards 0, will
be expressed by 2b ^ . In the same manner we prove, that the
attraction of a and c on b, in the direction bo, is ~^r- ; and that
of a and b on c, in the direction co, is ~cf • Hence, <2 6 and
£ being equal, the attractions in the directions ao bo and co will
also be equal ; and, consequently, in the direct ratio of these
distances. Or rather, the hypothetical attractions being equal, it
proves that, in order to revolve permanently, a b and c must be
equal to each other.
Instead of moving in one circular orbit, the three stars may
revolve in three equal ellipses, round their common centre of
gravity, as in Fig. 6. And here we should remark, that this
centre of gravity will be situated in the common focus 0, of the
three ellipses ; and that the absolute attraction towards that
focus, will vary in the inverse ratio of the squares of the distances
of any one of the stars from that centre, while the relative
attractions remain in the direct ratio of their several distances
of 500 new Nebula, and Clusters of Stars. 489
from the same centre. This will be more fully explained, when
we come to consider the motion of four stars.
A very singular straight-lined orbit, if so it may be called,
may also exist in the following manner. If 4 and b, Fig. 7, are
two large equal stars, which are connected together by their
mutual gravitation towards each other, and have such projectile
motions as would cause them to move in a circular orbit about
their common centre of gravity, then may a third small star c,
situated in a line drawn through 0, and at rectangles to the plane
described by the stars a b, fall freely from rest, with a gradually
acquired motion to ; then, passing through the plane of the
orbit of the two stars, it will proceed, but with a gradually re-
tarded motion, to a second point of rest d; and, in this manner,
the star c may continue to oscillate between c and d, in a straight
line, passing from ( , through the centre 0, to d, and back again
to c.
In order to see the possibility and permanency of this con-
nection the better, let be the centre of gravity of the three
bodies, when the oscillating body is at c ; then, supposing the
bodies a and b to be at that moment in the plane p I, and ad-
mitting m to represent a body equal in mass to the two bodies
a b, will be the common centre of gravity of m and c. Then,
by the force of attraction, the body c and the fictitious body m
will meet in ; that is to say, the plane p I, of the bodies a b,
will now be at p' V. The fictitious body m may then be con-
ceived to move on till it comes to n, while the body c goes to
d ; or, which is the same, the plane of the bodies a b will now
be in the position p" I", as much beyond the centre of gravity 0,
as it was on the opposite side m. By this time, both the ficti-
tious body m, now at n, and the real body c, now at d, have lost
4po Dr. Herschel's Catalogue
their motion in opposite directions, and begin to approach to
their common centre of gravity o, in which they will meet a
second time. It is evident that the orbit of the two large stars
will suffer considerable perturbations, not only in its plane, but
also in its curvature, which will not remain strictly circular;
the construction of the system, however, is such as to contain a
sufficient compensation for every disturbing force, and will con-
sequently be in its nature permanent.
In order to add an oscillating star, it is not necessary that the
two large stars should be so situated as to move in a circular
orbit, without the oscillating star. In Fig. 8, the stars a and b
may have such projectile forces given them as would cause them
to describe equal ellipses, of any degree of excentricity. If now
the small star c be added, the perturbations will undoubtedly
affect not only the plane of the orbits of the stars, but also their
figures, which will become irregular moveable ovals. The extent
also of the oscillations of the star f will be affected ; and will
sometimes exceed the limits c d, and sometimes fall short of
them. All these varieties may easily be deduced from what has
been already said, when Fig, 7 was considered. It is however
very evident, that this system also must be permanent ; since
not only the centre of gravity will always be at rest, but a 0,
whatever may be the perturbations arising from the situation of
c, will still remain equal to b 0.
It should be remarked, that the vibratory motion of the star c
will differ much from a cometary orbit, even though the latter
should be compressed into an evanescent ellipsis. For, while the
former extends itself over the diameter of a globe in which it
may be supposed to be inscribed, the hypothetical attractive
force being supposed to be placed in its centre, the cometary
of 500 new Nebulce, and Clusters of Stars. 491
orbit will only describe a radius of the same globe, on account
of its requiring a solid attractive centre.
After what has been said, it will hardly be necessary to add,
that with the assistance of any proper one of the combinations
pointed out in the four last figures, the appearance of every
treble star may be completely explained; especially when the
different inclinations of the orbits of the stars, to the line of sight,
are taken into consideration.
If we admit of treble stars, we can have no reason to oppose
more complicated connections ; and, in order to form an idea
how the laws of gravitation may easily support such systems, I
have joined some additional delineations. A very short expla-
nation of them will be sufficient.
Fig. 9 ( Plate XVII.) represents four stars, a b c and d, arranged
in a line; a being equal to b, and c equal to d. Then, if ao =
bo, and co = do, the centre of gravity will be in ; and, with a
proper adjustment of projectile forces, the four stars will revolve in
two circular orbits round their common centre. By calculating
in the manner already pointed out, it will be found, that when,
for instance, ao = 1, co = 3, and c = d = 1, then the mass of
matter in a = b, will be required to be equal to 1,34,92.
It is not necessary that the projectile force of the four stars
should be such as will occasion them to revolve in circles. The
system will be equally permanent when they describe similar
ellipses about the common centre of gravity, which will also be
the common focus of the four ellipses. In Fig. 10, the stars
abed, revolving in ellipses that are similar, will always
describe, at the same time, equal angles in each ellipsis about the
centre of hypothetical attraction ; and, when they are removed
from a b c d to a'b'c'd', they will still be situated in a straight
493 Dr. Herschei/s Catalogue
line, and at the same proportionate distances from each other as
before. By this it appears, as we have already observed, that
the absolute hypothetical force in the situation a' b' c' d', com-
pared to what it was when the stars were at abed, is inversely
as the squares of the distances ; but that its comparative exertion
on the stars, in their present situation, is still in a direct ratio of
their distances from the centre o, just as it was when they were
at a b c d; or, to express the same perhaps more clearly, the
force exerted on a', is to that which was exerted on a as
■=£=rr- : =^r . But the force exerted on a is to that exerted
on c, in our present instance, as ao = 1 to co — g; and still
remains in the same ratio when the stars are at a' and c' ; for
the exertion will here be likewise as a'o = 1 to c'o = 3.
Fig. 11 represents four stars in one circular orbit; and its
calculation is so simple, that, after what has been said of Fig. 5,
I need only remark that the stars may be of any size, provided
their masses of matter are equal to each other.
It is also evident, that the projectile motion of four equal stars
is not confined to that particular adjustment which will make
them revolve in a circle. It will be sufficient, in order to pro-
duce a permanent system, if the stars abed, in Fig. 12, are
impressed with such projectile forces as will make them describe
equal ellipses round the common centre 0. And, as the same
method of calculation which has been explained with Figs. 6
and 10 may here be used, it will not be necessary to enter into
particulars.
Fig. 13 represents four stars, placed so that, with properly
adjusted projectile forces, they may revolve in e^ual times, and
in two different circles, round their common centre of gravity 0,
of 500 new Nebula, and Clusters of Stars. 493
If ao = bo = 4, co = do=z 5, and c = c? = 1, then will the
mass of matter in a — b, required for the purpose, be 1,5136.
This arrangement, remarkable as it may appear, cannot be
made in all situations ; for instance, if the distance ao —bo were
assumed equal to 1, that of co — do being 2, it would be im-
possible to find such quantities of matter in a and b as would
unite the four stars into one system.
As we have shewn how the arrangement in Fig. 10 may be
derived from that of Fig. 9, so it will equally appear, that four
stars may revolve in different but similar ellipses round their
common centre, as in Fig. 14. For here the four stars, when
placed at abed, are exactly in the situation represented in
Fig. 13; but, on account of different projectile forces, they re-
volve, not as before in concentric circles, but in similar elliptical
orbits.
Fig. 15 represents three stars, a b c, in the situation of Fig. 5,
to which a small oscillating star, d, is added. The addition of
such a star to Fig. 1, has been sufficiently explained in Fig. 7;
and, what has been remarked there, may easily be applied to
our present figure. As the fictitious body m, in Fig. 7, was made
to represent the stars a and b, it will now stand for the three
stars a b and c. If we suppose these stars to be of an equal
magnitude in both figures, the centre of gravity 0, of the three
stars, will not be so far from m and n as in Fig. 7; and the
perturbations will be proportionally lessened.
Fig. 16 gives the situation of three stars, a b c, moving in
equal elliptical orbits about their common focus 0, while the
star d performs oscillations between d and e. What has been
said in explaining Fig. 8, will be sufficient to shew, that the
mdcccii. 3 S
494 D r ' Herschel's Catalogue
present arrangement is equally to be admitted among the con-
structions of sidereal systems that may be permanent.
We have before remarked, that any appearance of treble
stars might be explained, by admitting the combinations pointed
out in Figs. 5, 6, 7, and 8 ; and it must be equally obvious, that
quadruple systems, under what shape soever they may show
themselves, whether in straight lines, squares, trapezia, or any
other seemingly the most irregular configurations, will readily
find a solution from one or other of the arrangements of the
eight last figures.
More numerous combinations of stars may still take place,
by admitting simple and regular perturbations; for then all
sorts of erratic orbits of multiple flexures may have a permanent
existence. But, as it would lead me too far, to apply calculation
to them, I forbear entering upon the subject at present.
Before I proceed, it will be proper to remark, that it may
possibly occur to many, who are not much acquainted with the
arrangement of the numberless stars of the heavens, that what
has been said may all be mere useless surmise ; and that, possibly,
there may not be the least occasion for any such speculations
upon the subject. To this, however, it may be answered, that
such combinations as I have mentioned, are not the inventions
of fancy : they have an actual existence ; and, were it necessary,
I could point them out by thousands. There is not a single
night when, in passing over the zones of the heavens by sweep-
ing, I do not meet with numerous collections of double, treble,
quadruple, quintuple, and multiple stars, apparently insulated
from other groups, and probably joined in some small sidereal
system of their own. I do not imagine that I have pointed out
of 500 new Nebula, and Clusters of Stars. 495
the actual manner in which they are held together; but it will
always be a desirable step towards information, if the possibility
of such unions, in many different ways, can be laid before us ;
and, very probably, those who have more leisure to consider the
different combinations of central forces, than a practical astro-
nomer can have, may easily enlarge on what has been laid down
in the foregoing paragraphs.
IV. Of clustering Stars, and the Milky-way.
From quadruple, quintuple, and multiple stars, we are na-
turally led to a consideration of the vast collections of small
stars that are profusely scattered over the milky-way. On a
very slight examination, it will appear that this immense starry
aggregation is by no means uniform. The stars of which it is
composed are very unequally scattered, and show evident marks
of clustering together into many separate allotments. By referring
to some one of these clustering collections in the heavens, what
will be said of them will be much better understood, than if we
were to treat of them merely in a general way. Let us take the
space between j3 and y Cygni for an example, in which the
stars are clustering with a kind of division between them, so
that we may suppose them to be clustering towards two different
regions. By a computation, founded on observations which
ascertain the number of stars in different fields of view, it ap-
pears that our space between /3 and y, taking an average breadth
of about five degrees of it, contains more than 331 thousand
stars ; and, admitting them to be clustering two different ways,
we have 165 thousand for each clustering collection. Now, as
a more particular account of the milky-way will be the subject
of a separate paper, I shall only observe, that the above mentioned
3 S a
49$ Dr. Herschei/s Catalogue
milky appearances deserve the name of clustering collections,
as they are certainly brighter about the middle, and fainter
near their undefined borders. For, in my sweeps of the heavens,
it has been fully ascertained, that the brightness of the milky-
way arises only from stars; and that their compression in-
creases in proportion to the brightness of the milky- way.
We may indeed partly ascribe the increase, both of brightness
and of apparent compression, to a greater depth of the space
which contains these stars ; but this will equally tend to shew
their clustering condition : for, since the increase of brightness
is gradual, the space containing the clustering stars must tend
to a spherical form, if the gradual increase of brightness is to
be explained by the situation of the stars.
V. Of Groups of Stars.
From clustering stars there is but a short transition to groups
of stars ; they are, however, sufficiently distinct to deserve a
separate notice. A group is a collection of closely, and almost
equally compressed stars, of any figure or outline ; it contains
no particular condensation that might point out the seat of an
hypothetical central force; and is sufficiently separated from
neighbouring stars to shew that it makes a peculiar system of its
own. It must be remembered, that its being a separate system
does not exclude it from the action or influence of other systems.
We are to understand this with the same reserve that has been
pointed out, when we explained what we called insulated stars.
The construction of groups of stars is perhaps, of all the ob-
jects in the heavens, the most difficult to explain ; much less
can we now enter into a detail of the numerous observations I
of 500 new Nebula, and Clusters of Stars. 497
have already made upon this subject. I therefore proceed in my
enumeration.
VI. Of Clusters of Stars.
These are certainly the most magnificent objects that can
be seen in the heavens. They are totally different from mere
groups of stars, in their beautiful and artificial arrangement :
their form is generally round ; and the compression of the stars
shews a gradual, and pretty sudden accumulation towards the
centre, where, aided by the depth of the cluster, which we can
have no doubt is of a globular form, the condensation is such,
that the stars are sufficiently compressed to produce a mottled
lustre, nearly amounting to the semblance of a nucleus. A
centre of attraction is so strongly indicated, by all the circum-
stances of the appearance of the cluster, that we cannot doubt a
single moment of its existence, either in a state of real solidity,
or in that of an empty centre, possessed of an hypothetical force,
arising from the joint exertion of the numerous stars that enter
into the composition of the cluster.
The number of 'observations I have to give relating to this
article, in which my telescopes, especially those of high space-
penetrating power, have been of the greatest service, of course
can find no room in this enumeration.
VII. OfNebulce.
These curious objects, which, on account of their great dis-
tance, can only be seen by instruments of great space-pene-
trating power, are perhaps all to be resolved into the three
last mentioned species. Clustering collections of stars, for
instance, may easily be supposed sufficiently removed to present
4$8 Dr. Herschel's Catalogue
us with the appearance of a nebula of any shape, which, like
the real object of which it is the miniature, will seem to be gra-
dually brighter in the middle. Groups of stars also may, by
distance, assume the semblance of nebulous patches ; and real
clusters of stars, for the same reason, when their composition
is beyond the reach of our most powerful instruments to resolve
them, will appear like round nebulae that are gradually much
brighter in the middle. On this occasion I must remark, that
with instruments of high space-penetrating powers, such as my
40-feet telescope, nebulas are the objects that may be perceived
at the greatest distance. Clustering collections of stars, much
less than those we have mentioned before, may easily contain
50000 of them ; and, as that number has been chosen for an
instance of calculating the distance at which one of the most
remote objects might be still visible,* I shall take notice of an
evident consequence attending the result of the computation ;
which is, that a telescope with a power of penetrating into space,
like my 40-feet one, has also, as it may be called, a power of
penetrating into time past. To explain this, we must consider
that, from the known velocity of light, it may be proved, that
when we look at Sirius, the rays which enter the eye cannot
have been less than 6 years and 4^ months coming from that
star to the observer. Hence it follows, that when we see an
object of the calculated distance at which one of these very
remote nebulae may still be perceived, the rays of light which
convey its image to the eye, must have been more than nine-
teen hundred and ten thousand, that is, almost two millions of
years on their way ; and that, consequently, so many years ago,
* See Phil. Trans, for 1800, page 83. N. B. In the same page, line zz, for 5000
read 50000.
of 500 new Nebula, and Clusters of Stars, 499
this object must already have had an existence in the sidereal
heavens, in order to send out those rays by which we now
perceive it.
VIII. Of Stars with Burs, or Stellar Nebula.
Situated as we are, at an immense distance from the remote
parts of the heavens, it is not in, the power of telescopes to
resolve many phenomena we can but just perceive^ which, could
we have a nearer view of them, might probably shew them-
selves as objects that have long been known to us. A stellar
nebula, perhaps, may be a real cluster of stars, the whole light of
which is gathered so nearly into one point, as to leave but just
enough of the light of the cluster visible to produce the appear-
ance of burs. This, however, admits of a doubt.
IX. Of milky Nebulosity.
The phenomenon of milky nebulosity is certainly of a most
interesting nature : it is probably of two different kinds ; one of
them being deceptive, namely, such as arises from widely ex-
tended regions of closely connected clustering stars, contiguous
to each other, like the collections that construct our milky-way.
The other, on the contrary, being real, and possibly at no very
great distance from us. The changes I have observed in the
great milky nebulosity of Orion, 23 years ago, and which have
also been noticed by other astronomers, cannot permit us to
look upon this phenomenon as arising from immensely distant
regions of fixed stars. Even Huygens, the discoverer of it,
was already of opinion that, in viewing it, we saw, as it were,
through an opening into a region of light * Much more would
* See Systema Saturnium, page 8 and 9.
#oo Dr. Herschei/s Catalogue
he be convinced now, when changes in its shape and lustre have
been seen, that its light is not, like that of the milky-way, com-
posed of stars. To attempt even a guess at what this light may
be, would be presumptuous. If it should be surmised, for in-
stance, that this nebulosity is of the nature of the zodiacal
light, we should then be obliged to admit the existence of an
effect without its cause. An idea of its phosphorical condition, is
not more philosophical, unless we could shew from what source
of phosphorical matter, sUch immeasurable tracts of luminous
phenomena could draw their existence, and permanency ; for,
though minute changes have been observed, yet a general re-
semblance, allowing for the difference of telescopes, is still to be
perceived in the great nebulosity of Orion, even since the time
of its first discovery.
X. Of nebulous Stars.
The nature of these remarkable objects is enveloped in much
obscurity. It will probably require ages of observations, before
we can be enabled to form a proper estimate of their condition.
That stars should have visible atmospheres, of such an extent
as those of which I have given the situation in this and my
former catalogues, is truly surprising, unless we attribute to
such atmospheres, the quality of self-luminous milky nebulosity.
We can have no reason to doubt of the starry nature of the
central point ; for, in no respect whatever does its appearance
differ from that of a star of an equal magnitude ; but, when the
great distance of such stars is taken into consideration, the real
extent of the surrounding nebulosity is truly wonderful. A very
curious one of this kind will be found in the 4th class, No. 6q,
of the annexed catalogue.
of 500 new Nebula, and Clusters of Stars. 501
XL Planetary Nebula.
This seems to be a species of bodies that demands a particu-
lar attention. To investigate the planetary nature of these
nebulas, is not an easy undertaking. If we admit them to con-
tain a great mass of matter, such as that of which our sun is
composed, and that they are, like the sun, surrounded by dense
luminous clouds, it appears evidently that the intrinsic bright-
ness of these clouds must be far inferior to those of the sun. A
part of the sun's disk, equal to a circle of 15" in diameter, would
far exceed the greatest lustre of the full moon ; whereas, the
light of a planetary nebula, of an equal size, is hardly equal to
that of a star of the 8th or 9th magnitude. If, on the other
hand, we should suppose them to be groups, or clusters of stars,
at a distance sufficiently great to reduce them to so small an
apparent diameter, we shall be at a loss to account for their
uniform light, if clusters ; or for their circular forms, if mere
groups of stars.
Perhaps they may be rather allied to nebulous stars. For,
should the planetary nebula? with lucid centres, of which the
next article will give an account, be an intermediate step be-
tween planetary nebulas and nebulous stars, the appearances of
these different species, when all the individuals of them are fully
examined, might throw a considerable light upon the subject.
XII. Of planetary Nebula with Centres.
In my second catalogue of nebulas, a single instance of a
planetai-y nebula with a bright central point was mentioned;
and, in the annexed one, No. 73 of the 4th class, is another of
very nearly the same diameter, which has also a lucid, though
mdcccii. 3T
£oa Dr. Herschei/s Catalogue
not quite so regular a centre. From several particularities
observed in their construction, it would seem as if they were
related to nebulous stars. If we might suppose that a gradual
condensation of the nebulosity about a nebulous star could take
place, this would be one of them, in a very advanced state of
compression. A further discussion of this point, however, must
be reserved to a future opportunity.
CORRECTION OF A FORMER PAPER.
In my Paper on two lately discovered celestial Bodies,
Page 224, line 18, of this volume, instead of 135, read -31.
oj 500 new Nebula, and Clusters of Stars,
$°S
Catalogue of 500 additional new Nebula, and
Clusters of Stars.
First Class. Bright Nebula.
I.
1788.
Stars.
M.
s.
D. M. %
i Description.
216
Dec. 3
22 Ursge
P
13
5*
/
3 4 s
s ^B.^L.z'F.r.w^M. Towards
the ff within the nebulo-
sity, is a f S. /£.
217
27
54 Persei
f
9
25
n
46 s
5 cB. cL. mbM. Stands nearly
in the center of a trape-
zium.
218
Si
1789
63 Auriga*
f
2,6
43
I
O 20 1
cB. R. vgmbM. about %'d.
219
Mar. 23
55 Ursa?
I
5
33
n
O 361
vB. cL. iF. vgmbM.
220
Apr. 12
64 (q/) Ursas
P
43
.59
J
20 S
1 cB. mE. 70 np ff. 3 or 4' /,■
221
_
— —
P
21
4 1
I
O 37 s
j cB. R. vgmbM, 4 or 5'^.
222
_
— —
P
20
20
I
35 s
i cB. z'E. near mer. g&M. 2'/.
223
—
— —
I
6
4
I
2 45s
i z>B. mE. »/> ^: BN. 5'/. ii'6.
224
—
1 Canum
P
9
13
I
3 10s
JcB.^L.mE. SN.
225
—
— —
P
8
3i
I
46j£
t i>B. pL. BrN. just/ a r/5f.
226
14
64 [y) Ursse
P
33
32
I
34' 1
cB.R.SBrNandrFchev. tfd.
227
— ^ —
P
15
28
n
3 37| s
1 cB. cL. iF. r. vgbM. g'l. v'b.
228
—
— —
P
5
20
n.
2 24s
1 vB. vBiN. and F. bran. i±'h
i'b.
The 2d of 2. vB. R. vgbM.
229
_
_ __
f
3
46
n
i 47 3
See II. 791.
230
— —
83 Ursee
f
20
24
n
27 s
>.cB. S. E.y/> «/. cBN. and F
bran.
231
—
— —
f
24
34
n
10s
s cB. />S. iR.
232
■ "
■ " ' ' "
f
27
7
n
16 j
The adofa.cB.S.R.tg-m&M.
See III. 791.
233
V7
44 Ursee
I
1
14
I
16 s
i cB. E. 30°^ nf.r. mbM. 3'/.,
3 T 2
504<
Dr. .Herschei/s Catalogue
I.
1789.
Stars.
M.
s.
M. D
£ Description.
234
Apr. 1 7
74 Ursae
/
1
31
/
O 28'
2 cB. S. /E. Just^> a phft.
235
—
12 (-*) Draconis
P
66
52
/
2 3<.
1 cB. iF vgmbM. 7' /, 5' b.
236
—
— __
P
59
56
I
2 13.
$vB. S. z'R. Bz'rN. vgmbM.
237
—
_ ' —
P
54
10
/
O 52
1 B. z oval. vgmbM.
238
24
69 Ursae Hev.
I
27
55
/
32$
1 cB. ph. iR vgmbM.
239
—
— —
f
28
10
/
17gcB.pL. E.mbM.
240
—
— —
J
28
34
/
ty^cB.pL.E.SBN.
1790
241
Feb. 17
19(g) Hyd.Crat.
P
H
43
/
57 1
l cB. E. 70 «/>^f. vgbM 7'/,
4'6. within a parallelo-
gram.
242
Mar. 17
15 (/) Ursae
P
15
4°
/
21 1
vB. LBrN. with vF chev.
243
—
77 (e) Ursa?
I
1
47
n
2 251
1 cB. S. R. gbM.
244
18
39 Ursae
f
36
44
n
40 s
.cB.R. vgmbM. i±'d.
®45
—
— —
I
39
27
n
1 58£
> vB. cL. R. vgbM.
246
—
66 Ursae -
P
29
19
n
20 s
.cB.ph.E.
247
__
— —
P
28
*3
n
2 OS
1 vB.pL. IE. near par. mbM.
248
—
— —
P
7
5
n
2 52 s
uB.p'L.iF.
249
19
1 7 Ursae
P
9
n
3 43 s
> cB E. near par. er. bM. 4' /,
2' 6. I suppose, with at
higher power and longer
attention, the stars would
become visible.
250
—
— _
P
4
47
n
3 17 ]
1 vB. cL. IE. LBNM.
251
,
76 Ursae
P
50
48
I
2 31
vB. perfectly R. BN and F
chev. vgbM. \\' d.
252
—
_ —
P
41
ji
I
34 1
vB. cL. R.
253
—
— —
P
41
46
J
51 1
vB. vh. E.
254
P
1
47
I
1 81
eB. E. par. 5' I. all over
equally B. except just on
the edges.
255
—
69 Ursae Hev.
f
19
26
n
1 1 1
vB, BENM. 3' /. \> b.
256
—
— . —
I
21
33
n
13]
vB.ph. iF. suddenly mbM.
257
Oct. 9
12 Eridani
I
16
58
I
1 581
cB. iR vgmbM. i±'d.
258
Dec. 28
47 (a) Persei
P
3
41
n
1 O]
vB.iF.r.bM.s'l.^'b.ApL
star in it towards the f
side, but unconnected.
of 500 new Nebula, and Clusters of Stars.
505
I.
1791.
Stars.
M.
s.
D. M. «
1 Description.
259
Mar. 7
17 Hydras Crat.
/
18
3 1
ra
O 27]
cB.p~LJE.gbM. Thebright-
ness takes up a large space
of it.
260
Apr. 2
*793
23 (b) Ursa?
P
1
49
/
34'
vB. vS, iR. mbM.
261
Feb. 4
38 of the Connois.
f
3
7
/
1 35i
vB. iR. vgbM. s'd. Seems
to have 1 or 2 stars in
the middle, or an z'N ; the
chev. diminishes vg.
262
Apr. 6
1 (x) Draconis
P
2
6
/
2 41 1
cB. vS. iF. N. with vF. chev.
263
—
4 Draconis -
P
22
48
J
231
cB. IE. bM.
264
7
— —
P
*4
18
n
1 36*1
cB. S. 6M.
265
8
37 Ursse
P
16'
16
n
1 51
cB. S. /R. vgmbM.
266
— - .
— —
P
13
35
J
11 1
cB. ph. iF. gbM.
267
39 Ursse
f
11
21
I
10 1
cB.ph. iR. i±'d.. The great-
est part of it almost e-
qually B.
268
—
— —
f
12
46
f
41
vB. vS. R. Stellar.
2%
—
— —
f
18
1
n
29 1
cB. R. 1 'd. just n of a Sft.
270
— .
_ — 1
f
35
2,6
n
1 42 s
s vB. ch. E. par. SN. E par.
271
—
— —
f
35 54
n
551
. v B. ch. E. mbM.
1796
272
Mar. 4
Georgian planet
P
53
n
6 s
icB.S.iR. BN.mbM. This
nebula was seen at g h 27',
sidereal time; the tele-
scope being out of the
meridian.
373
Nov. 22
A double star
f
. 5 45
I
891
) vB. vh. E. near par. The
determining star follows
5DraconisHevelii 13' 54"
in time, and is o° 23' more
south.
274
—
'__ _ —
I
10
13
I
24?
j cB. vS. *R, bM.
275
Dee. 10
5 Dracon. Hev.
f
1
32
11
12s
1 cB. S. R.
276'
—
_ _ —
f
2
45
n
12s
1 cB. ch. iF. IE. mbM.
277
—
— —
J
6
20
n
O 20 5
1 vB. ch. IE. mbM.
278
12
— —
P
11
5
J
O 15^
icB.ch.iR. mbM.
§oS
Dr.
H
ERSCHEI
's
Catalogue
i.
1796.
Stars.
M. S.
D. M.J
> Description.
®79
Dec. 12
— — - — —
P
IO 28
n
1 38 2
cB. cL. /E. 6M.
280
1798
i6(£)Ursa2min.
f
51 33
n
$i
• »B. dL. /E. #>M. The great-
est brightnes confined to
281
Dec. 9
t Apps. Sculps.
!
a small noint.
L.C.95 -
P
1 47
n
O 27 1
cB. E. np ff. NM. Q'l. i%h.
1801
282
Apr. 2
2o8(N)Camelop.
of Bode's Cat.
P
i53 15
1
2 43 1
cB. ph. z'F.
283
—
— —
P
113 40
1
3 4 1
cB. cL. er.
284
—
. -»_ —
P
85 18
J
23 5
cB. pS. z'F.
285
Nov. 8
24 (d) Ursas
J
13 14
J
1 53 5
vB. vL. E. a^. 6'/. Q'b.
286
f
3° °
J
1 8i
. vB. cL. R. vgmbM. On the
north-following side there
is a F ray interrupting the
roundness.
287
Dec. 7
1802
1 (a) Draconis
P
4 37
n
1 131
cB. mE. np Jf. mbM. 3'/, l'b.
288
Sept. 26
184 Camelopar.
*
J of Bode's Cat.
P
n 58
J
2 34
1 vB. cL. IE. suddenly mhM.
Second Class. Faint Nebula.
11.
1789.
Stars.
M. S.
D. M. ;
r Description.
7%
Feb. 22
81 [g) Geminor.
P
37 58
n
O 4
1 pB. pL. iR. er. bM.
770
—
62 Ursaa
P
13 44
J
2 15-
1 pB. pL. R. IbM.
771
Mar. 20
2 ^'(%) Virginis
P
7
n
O 26'!
2 pB. cL. z'F. *r. w6M. 4 or 5'd.
772
—
— —
f
3 9
n
57-
i F. S. E.
773
—
— —
f
3 5
n
1 i ;
2 F. S. E. bM.
774
"""■"
— _
f
6 27
n
55 c <
i pB. S. iR. mbM,
775
23
55 Ursse -
f
3 S.i
J
25-
i pB. cL. IE. vgmbM.
776
26 (%) Virginis
P
8 19
J
4
1 F. pL. er.
777
• __
— . —
I
17 ] 5
n
1 9'
t F. S. R. 6M.
778
— —
f
21 12
n
1 54
i F. S. //". a double star.
779
16 (%) Virginis
f
22 44
n
14
1 F. S.
780
26
46 ( 7 ) Hydrae
f
1 22
I
1 14J
1 F. R. r. vglbM. 4V.
of goo new 'Nebula, and Cluster* of Stars.
507
II.
1789.
Stars.
M. S.
D. M.
y Description.
781
Apr. 12
1 Canura -
P
10 55
/
53'
2 ApS.ft. involved in nebu-
losity of no great extent ;
theft, does not seem to
belong to it.
782
H
64 (y) Ursas
P
31 7
n
7
1 pB. S. R. vgmbM. just fa
Sft.
783
—
— —
P
18 40
n
50
i pB. ph. bM.
784
—
— i —
P
17 4»
n
37 •
1 pB. ch. IE. 2>'l
785
—
— - _—
P
7 3
n
2 18:
ipB. S.-/E.
786
—
— —
P
3 31
n
1 39
F. E.
787
}-
P
3 2
W
1 27.
r Two nebulae; the ist^B. S.
l lThe2d^B. S.
788
3 7
it
1 24
789
790
}-
— —
I
1 25
n
1 38:
r Two nebulas; the 1 stpB. E.
1 1 The 2d F. S.
791
—
, __ . —
f
3 3 4
n
1 483
i The 1st of 2. pB.S.E. See
I. 229.
792
—
1 Canum -
P
3 12
n
3 47"
t F. S. R. bM,
793
—
— _
P
57
n
2 365
1 F. pL. i¥. bM.
794
—
77 (e) Ursa?
P
11 32
J
49 s
1 F. S.
795
—
— — -
P
8 25
J
1 13 s
j j&B. v S. m&M.
796
—
— ■ _.
P
7 20
I
1 25 s
j />B. cS. /E. BrN.
797
—
8 1 Ursas
P
3 33
f
2 18s
j />F. pS. R. t^M.
798
—
83 Ursas -
J
49
n
111
/>B. E. ii'/, f6.
799
—
— —
f
21 27
n
1 7 s
j />B. cL. E.
800
—
. . — ■ —
I
25 7
n
1 2 ]
1 pB. S.
80 1
—
— . _. ■
1
27 27
n
23 s
5 F. cL.
802
17
71 Ursas -
P
15 20
n
1 331
F. S. E.
803
— —
P
*3 57
n
59 s
s F. S. R.
804
—
— —
P
5 43
J
31
/>B. />L. z'F.
805
— •
— • —
P
4 41
n
1 201
The 2d of 2./>B./>L. w6M.
See III. 798.
806
—
— _.
P
2 13
n
1 42 J
/>B.
807
—
i2(<) Draconis
P
55 48
n
42 1
/>B. E. mer. \\'l, |6.
808
24
Neb. II. 756
P
24 16
n
41 i
1 />B. S. z'F. er. mixed with
some/>L. stars, which may
perhaps belong to it,
809
"™*
- — — _ ■
P
15 5
J
263
F. S. E.
5 o8
Dr. Herschei/s Catalogue
II.
1789.
Stars.
P
M. S.
D. M
Description.
8io
Apr. 24
21 ([a.) Draconis
4 6> 3i
n
3 3 3
1
/>F. pS. IE.
811
—
— —
P
44 9
n
50
1
pB. z'R. vgvlbM.
812
- —
- — —
I
10 4
n
2 55
1
F. S. R. ^/6M.
813
26
5 Canum
P
10 53
I
50
1
/>B. S. IE.
814
- —
7 Canum
I
20 24
n
1 20
1
F. S. tj/k6M.
815
—
82 Ursa?
P
3 1 48
I
52
1
F.t>S. Stellar.
816
—
— . —
P
9.6 52
J
1 36
1
F. S. zR. vgmbM.
817
—
— —
P
3 4 2
I
1.4°
1
pB. S. R. ^6M.
818
1790
12 Draconis
P
40 16'
n
33
1
pY. c$. R. i>#6M.
819
Mar. 8
ig{x)Hyd.Crat.
P
11 58
n
31
1
/>F./L. iF. bM.
820
10
65 Auriga?
f
7 22
n
1
1
pB. S. Stellar.
821
—
7oGeminorum
P
1 43
n
12
1
pB. cS. r. p a eft.
822
n
27 Lyncis -
P
25 42
n
41
1
pY. R. r. vgbM.
823
15 (I) Ursas
P
12 10
J
18
1
pB. S. R. w&M.
824
—
26 Ursae -
f
*39 17
J
1
1
/>B. mE. 67, 2'6.
825
_
— —
J
139 40
J
1 44
1
/>B. S. fF, 6M.
826
—
77 (s) Ursas
f
28
n
1 42
1
F. S. E.
827
—
— —
I
69 59
n
3 27
1
pB. S. z'F. mbM.
828
18
17 Ursaa
P
6 25
J
2 57
1
pB. S. vgmbM.
829
—
66 Ursa?
P
3i 14
n
1 9
2
Y.E.npff.er.ii'l.
830
—
— — .
P
15 23
I
20
1
pB. E.
831
—
— —
P
11 44
n
1 22
1
/>B. r;S. IE.
832
P
6 53
u
2 52
2
pB.pL. R. The nebulosity
of this runs into that of
I. 248.
833
—
. :
P
1 1
n
1 4 6
1
F. S.
834
19
17 Ursaa
P
11 34
n
3 10
1
pY. pS. iY. er.
835
—
29 (u) Ursa?
J
5 "
n
15
2
F. S. E. near par.
836"
—
76 Ursaa
P
70 41
I
53
1
F. S. R. r. almost of equal
light throughout.
837
—
— . —
P
66 54
J
1
1
pB. IE.
838
—
— —
P
66 15
J
3 9
1
pB. S.
839
—
— —
P
63
J
2 28
1
pB. cS. R. mbM.
840
—
— . — _
P
47 3o
J
2 16
1
Y. S. bM.
841
—
69 Ursas Hev.
I
4 24
n
2 46
2
The 1st of 2. pB. S. iY.
842
—
— —
J
4 35
n
2 50
2
The 2d of ^. pB.pl,. iY.
of 500 new Nebula, and Clusters of Stars.
509
II.
1790.
Stars.
M. S.
D. M.
42
Description.
843
Mar. 19
__ _ _
/
26 40
n
iF. S.
844
— .
— . —
J
2 7 43
I
29
1 pB. cL.
845
20
50 («) Ursae
/
22 41
n
1 44
3 pB.pL. z'R. bM.
846
—
76 Ursas -
P
23 9
n
3 13
1 pB. mE.fpnf. BN. gl,±'b.
847
— —
P
19 1
n
3 8
1 pB. S. IE.
848
—
— —
P
14 Q i
n
2 8
1 F. iF. bM. Stellar.
849
—
— —
P
9 7
n
1 15
1 pB. vS. IE. SN.
850
—
— , —
P
7 16
n
48
1 pB. ph. iR. r. vgbM.
851
Oct. 9
72 Pegasi
I
18 3
I
6
2 pF.ph. iR. IbM.fp.avSft,
852
—
o- Fornacis L. C.
285 - -
P
4 *5
I
34
iF.ph.iR.gbM.
853
Nov. 26,29 (tt) Androm.
P
25 3 8
J
24
1 F. S. E. nearmer.
854
Dec. 25
44 Piscium -
f
3 49
n
56
1 pB. vS. R. vgmbM. pretty
well defined on the mar-
855
— ;
— —
I
4 44
n
10
gin.
2 pB. ch. iR. r. vgbM. fp. a
vSJt.
856
—
— —
f
13 52
n
1 8
1 F. S. vgbM.
857
—
— —
J
13 52
n
53
1 F. S. vgbM.
858
—
— —
f
14 10
n
58
1 pB. S. vgbM.
859
—
98 (jt*) Piscium
I
20 28
n
1
1 pB S. E. near par.^fr. a S/£.
860
28
Mayer's Zod.
Cat. No. 18
P
5 4 8
n
39
1 pF. vS. vgbM.
861
—
57 Auriga? -
J
17 30
n
1 54
1 pB. ph. iF. gbM.
862
—
— ' —
f
23 5
n
1 29
iF.pL.
863
2 .9
63 ($) Piscium
P
39
n
44
1 ph. IE. r. gbM.
864'Mar. 7
17 Hyd. Crat.
f
16 46
s
1
1 pB, S. R. vgmbM. almost
resembling a N.
8%
866
r Two nebulas, both F. S. R.
}-
— — -
f
34 2
J
3 1
1 1 bM. and nearly in the
[ same par.
867
April 2
73 Ursa?
P
14 8
I
1 12
1 pB. vS. Stellar.
868
10 38
11 8
r Two nebulse, the 1st F. S.
86 9
} 8
14 (t) Ursae
f
n
47
1 iF.
J
J
[The2dF.*L.E.
1
MDCCCII,
3 U
£10
Dr. Herschei/s Catalogue
ii.
870
April 3
874
875
1791.
35 Ursa? -
871
872
873 May 6
Stars.
3
1792
876 Apr. 20 22 (f) Bootis
877 - _ _
878 Sept 16 3CepheiHev.
1753
879 April 6
880
881
3 (yjUrsasmin.
24 37 (I) Bootis
;o 25 Herculis
7
882 8
883
884
885
886
887
888
889 May 1 2
890
891
892
893
894
895
896
897
898
1 (a) Draconis p
P
4 Draconis
37 Ursa?
39 Ursa?
942 Ursa?
19 Bootis Hev.
/
/
/
/
/
/
P
P
i393( T )Virginis
Sept. 6 53 Aquarii
1794
Georgian planet
P
f
I
J
I
I
P
P
I
I
I
I
P
P
J
M. S.
2 50
3 37
21 gO
37 53
34 4 8
3 10
1.5 58
13 27
29 1 5
9 49
/
/
n
I
I
n
n
n
I
I
D. M.
7 44 M
45 43 n
o 12
10 40
8 36
22 42
37 41
44 5
2 41
7 21
26 45
13 20
6* 44
7 44
9 37
10 46*
21 54
21 49
16 29
3 °
n
n
I
n
I
n
n
11
n
n
n
\
n
n
o 3 6
o 52
11
1 17
1 12
2 12
26
1 21
o 25
3
8
37
42
2
56
11
20
33
8
24
22
31
40
40
7i
Description.
F. S. iR. Almost of equal
light throughout.
F. vS. mbM.
F. cL. iR.
F. R. 6M. i'd.
pB.ph. iR. vgmbM,
pB.S. IE. vgmbM.
o 33
vS.
pB. ph. iF.
pB. iF.bM. contains 2 stars.
pB. S. R. bM.
F. S. /E. fp nf. but near
mer. gbM.
F. wE. «/>^. but near par.
if/.
pB.pL.lE.bM.
F. S. R. bM.
F. S. R. 6M .
F. S. /E. w/)^.
/>B. iF.
F./>L. /F. bM.
F. S. R. 6M.
pB. pL. R. just foil, a S/t
/>B. />L. z'R.
pB. ph. IE. BM.
F. S. E. near mer.
pB. S. iF.
F. S.
F. S. iR.
F. S. ?R.
^B. IE. r. if/, if 6.
F. 3' north of a />L. red ft.
This nebula was seen at
8 h 49', sidereal time, the
of goo new Nebula, and Clusters of Stars.
£11
II.
1797.
Stars.
—
M. S.
D. M.
a*
Description.
telescope being out of the
meridian.
$99
Dec. 20
1798
4t(b) Urseemin.
P
26 13
/
40
1
F. S. E, near mer. i'I.
9 00
Dec. 10
1799
18 (e) Eridani
P
20 53
y
1 5
1
F. E.fp nf. near par. 3'/, x'b.
901
June 29
93 Herculis -
P
2:7 30
/■
11
1
F. S. i¥. er. 2'/.
902
1801
— . —
I
7 47
n
49
1
F.^L. R. vgbM.^'d:
9°3
April 2
2o8(N)Camelop.
of Bode's Cat.
P
139 19
f
1 39
1
F. pL. r.
904
—
— —
P
6"8 9
1
1 5 8
1
F. pL. IbM.
905
—
. _*_ —
P
3 6 53
!
2 22
1
pB. ph.
gob
Nov.28
1802
11 (a)Draconis
I
86 13
n
8
1
F. 8. lE.fpnf.vglbM.
907
June 26
2 (p) Lyraa
f
5 21
n
18
1
F. S. *F.
jfi6z'rd C/ass. Very faint Nebula.
III.
1788.
Stars.
M. S.
D. M.
Description.
748
Dec. 3
43 Camelop.
/
35 5
w
29
1
»F. z>S. has a vF. bran «/.
749
. —
22 Ursas
/>
12 45
./'
24
1
6-F. z>S.
75^
3i
63 Auriga? -
./
48 58
re
4,3
i
vF. S. R. /6M.
75i
1789
39 Lyncis -
/
25 15
y
30
2
*F. S.
752
Feb. 22
16 (£") Cancri
P
4 19
n
8
1
eF, IE. f of sl v$ft.
753
—
33 ( r ) Cancri
P
8 11
1
4
1
vF. S. R. v/&M.
754
24
6 Corvi
P
17 33
/
1 43
1
^F. wS. R.
755
756
"iMar.
J 2 °
f Two nebulae, both t>F. vS.
26 (%) Virginis
P
13 3
»
so
1
•j E. within if of each
I other.
757
-
P
5 25
n
38
2
2 vS. stars involved in »F.
nebulosity of no great ex-
tent.
3U 2
513
Dr. Herschei/s Catalogue
III.
1789.
Stars.
M. S.
D. M. <
3 Description.
758
759
->Mar.
J 23
— . —
/
SO 55
n
1 53
1 Two nebulas, both vF. vS.
760
—
_ __
/
23 47
I
9
1 cF. vS. R.
761
—
— —
/
24 55
n
18.
1 vF. S.
762
—
102 (u')Virginis
P
11 30
n
36
1 vF. vS.
7^3
—
10 5(<p) Virginis
P
1 1
I
1
t eF. S.
7^4
26
9 (0) Corvi
P
4 55
n
15 ■
1 cF. pS. R. Stellar.
765
—
45 (40 Hydra
P
1 35
I
53
ivF.pL. z'F.
766
___
— _
J
39
I
16' ■
1 i>F. » S.
767
Apr. 12
64 (y) Ursse
P
78 24
J
3 45i
i vF. p$. i E.
768
—
— —
P
30 48
J
49 s
$z>F. vS. Stellar.
769
—
— —
P
1 40
I
1 44]
t cF. S.
77o
14
—— .— — .-
P
39 3 2
n
2 2 :
1 vF. vS. Stellar.
77i
P
19 37
n
1 8
i<?F. S. z'E On account of
the brightness of 1 yg Ur-
sae maj. of Bode's Cat.
which was in the field of
view with it, I had near-
ly overlooked it.
772
— .
__ . — .
P
19 2
n
1 16 ]
.vF. Stellar.
773
—
— —
P
14
n
2 32 1
uF.pS. ZE. just/ a vS/f.
774
—
— ■ —
P
10 37
f
58 s
svF. S.
775
—
__ —
P
10 17
I
1 1 ]
1 vF. vS.
776
—
. — __
P
9 33
n
2 12 ]
1 eF. pL. IF.
777
, — .
1 Canum -
P
1 54
/
331
ieF. S. Stellar.
778
— ■ ,
77 (e) Ursas
t
9 10
i
1 4s
icF.S.lE.iF.
779
— ,
— __
f
11 36
n
20 s
*t>F. S.
780
— .
— __
I
12 37
I
19]
1 cF. S.
781
782
}-
— , __
J
12 30
12 44
I
2 22
2 20 '
t j Two nebulae. Both vF. S.
7 8 3
—
— . —
I
12 33
J
2 28 :
1 vF. S. E.
784
—
81 Ursaa
P
7 6
n
9
1 cF. S. zR.
785
—
83 Ursas
I
4 34
n
37
1 2 <?F. ft. with nebulosity.
786
__
— , — ,
f
14 3
J
22
lfF.f'S. Stellar.
787
—
— . —
I
22 27
J
28
1 vF. vS.
788
. —
— , __
f
23 47
I
24
1 f F. vS.
789
"
ft*™* 1 .mi .1 1,
f
23 54
I
22
1 vF. vS.
of 500 new Nebula, and Clusters of Stars.
5*3
III.
1789.
Stars.
M. S.
D. M. 5
r Description.
790
Apr. 14
83 Ursse
/
25 23
/
O 171
vF. pL.
791
—
/
27 7
n
O 16 1
l The 1st of 2. vF. S. 4'dist.
from I. 232.
7.92
17
44 Ursse
P
2 11
n
50 ]
v F. S. E. 20°^5> nf. er.
793
48 (jG) Ursse
I
1 25
I
O IOI
vF. vS. Stellar. The bright-
ness of jS Ursse is so con-
siderable, that it requires
much attention to perceive
this nebula.
794
—
71 Ursse
P
22 30
n
1 8i
cF. S. ver30o»
795
—
— —
P
16 8
n
2 52
, vF. S. iF. r«
796
—
— —
P
11 23
n
2 52 J
eF.
797
—
_ —
P
P
10 56
n
3 11S
s vF. S.
798
—
_ — .
5 4
n
1 20]
1 The 1st of 2. cF. IE. iF. II.
X
805.
799
, —
— . —
P
P
1 12
n
1 361
1 t>F. v S.
800
801
}-
— —
1 9
n
I 371
r Two nebulse, both eF. cS„
1 I R.
802
___
74 Ursas
f
4 54
n
O 3OS
j The 1st of 2. vF. S. /E. See
III. 807.
803
—
69 Ursse Hev.
f
9 33
I
2 53 c -
j eF. fS.
804
—
— —
J
46 59
I
2 18s
s eF. S. E. r.
8o 5
—
— — ,
f
48 9
I
1 1
5 eF. vS. R. Stellar.
806
—
i2(<) Draconis
J
P
34 20
n
8i
1 1> F. z> S. IF.
807
24
74 Ursse
I
5 26
n
34
1 The 2d of 2. eF. S. E. diffe-
rently from III. 802.
808
—
69 Ursse Hev.
P
7 35
I
2 19]
1 cF. S. E.
809
—
— —
f
27 7
I
1 25]
1 vF. vS.
810
—
— —
I
30 44
f
13
1 cF. vS. R.
811
—
Neb. II. 756
f
32
n
2 ]
LfF.S.E.
812
— ,
21 (p) Draconis
P
55 20
n
3 18]
1 vF. vS. IE.
813
—
— —
P
36 1
n
1 14-
1 z>F, vS. *'R.
814
26
5 Ganum
P
15
n
32-
1 z>F. S. er.
815
—
7 Canum
f
18 48
f
22 •
1 S. Stellar.
816
— —
f
25 11
n
* 33'
1 eF. S. ZE.
817
—
— —
I
26 43
n
45
l cF. S. *F.
818
—
— —
f
33 4
I
1 7
1 cF. S. R. i^/6M.
SH
Dr. Herschel's Catalogue
in.
819
820
821
822
823
824
825
826
827
828
829
830
831
832
833
834
835
836
837
838
839
840
841
842
843
844
845
846
847
848
849
850
1790
Mar. 8
1789.
Apr. 26'
82 Ursa?
10
17
18
Stars.
7(«)Hyd.Crat.
39 Lyncis
Hyd. L. C. 1039
;7 Lyncis
15 (f) Ursa?
26 Ursa?
74 Ursa?
77 Ursa?
17 Ursa?
43 Ursa;
66 Ursa?
69 ($) Ursa?
19 20 Ursse
76' Ursa?
69 Ursa? Hev.
20 76 Ursa?
P
P
P
f
P
P
I
P
P
P
P
I
P
P
P
P
P
P
P
P
P
P
I
P
P
f
P
M. S.
33 15
29 17
12 59
6 23
5 5
7 26
12 1
5 55
2 11
2 1
23 49
10 40
12 8
9 39
*34 3
2 4
82 37
79 17
75
75
72
63
16
5
19
16"
4
7
S7
19
23
26
32
10
/
22!/
56\f
if
8
23
1
53
53
5
53
56
D. M.
12
48
7
25
1
9
3 1
56
29
11
30
19
23
57
43
56
52
40
15
40
28
9
39
52
2
17
23
50
13
8
17I1
Description.
vF.
2fS stars at less than l'd.
with f F. nebulosity be-
tween therm.
cF. Stellar.
cF.pS. ill. IbM.
cF.pL.R.vlbM.
vF. vS. z'R. glbM.
vF.S.R.bM.fofaSft.
vF. S r.
eF.vS.ffavSft.
eF.pS.R.vgbM. Stellar. just
p a t>S/£.
eF. wS. R. bM.
cF.pS.bM.
vF. v$.
vF. S. IE.
vF. vS.
eF. S. zF.
eF. S. E. but nearly R.
t^F. vS. maybe a patch of
stars.
eF. v S.
eF. z>S.
eF. wS.
cF. cS.
vY.S.
vF. vS. R.
f F. Stellar, np a S/h
z^F. S. mE.
t'F. S. E. par.
cF. S. mE. very narrow.
eF. v S. zF.
t;F. f S.
z>F. z>S.
|vF./>S.
of 500 new Nebula, and Clusters of Stars.
&-i
III.
1790.
Stars.
M. S.
VI. D. a
Description.
851
Mar. 20
y6 Ursas
P
25 25
n
3 43 *
*F. S. iF.
852
— -
— — __
P
l6 38
n
3 12 1
vF. Stellar, nfa S triangle of
Bft.
853
Apr. 1
go (<p) Ursas
f
8 55
n
1 35 ^
vF. S. vglbM.
854
Oct. 9
72 Pegasi
f
15 8
J
D 232
qvS close ft. with nebulosity
between.
%5
S56
f Two nebulas, both eF. Stel-
| lar. dist. l'from 30°^*
I to nf.
}-
— —
f
27 *5
n
O 3:: 1
857
7 Fornacis L. \
C. 285 - J
P
12 30
I
1 54 1
vF.S.iF.lbM.
858
10
6 Pegasi -
P
24, 40
n
43 1
eF. pL. ill. vlbM. requires
great attention to be seen.
859
—^
__ _
P
7 S^n
171
l cF.vS.iR.mbM.nea.ra.vSft,
860
Nov. 2
72 Pegasi
P
5 ] 9»
1 71
vF. S. IbM.
861
,-—
— —
f
37 5o
I
171
. eF. S.
862
8
1 Lacertas Hev.
P
3 17
n
1 19 1
£>F.jbL.z'R. r.
863
—
— —
f
3 9
n
481
. vF. vS. mbM.
864
—
— . —
f
4 37
n
50 j
. vF. S. raE. 75 ȣ/jf. 6M.
865
13
26 Auriga?
P
1 9
n
1 311
t z>F. vS. R- 6M.
866
26
29 [mr) Androm.
P
27 37
I
20 '
l f F. r>S. The «£ corner of a
square.
867
Dec. 6
Mayer's Zod.i
Cat. 20 - 1
P
49 5 9
I
1 39
ieF.pS.iR.lbM.
868
—
— —
P
39 35
I
42"
ieF.pS.iF.
86c,
25
4,4, Piscium
f
3 25
n
55
t vF. vS. bM. p. and in the
field with II. 854. nf. 2.
Sjt.
870
, — ,
— —
f
12 48
n
49
1 vF. S. zR. vgbM.
871
28
Mayer's Zod. i
Cat. 1,8 - J
P
8 1
n
1 44
1 vF. S. R. vgbM.
872
,
— . —
P
5 52
n
41
1 i>F. riS. 6M.
873
~ ~
P
5 3 2
n
39
1 ^F, cL. In the field with the
foregoing, and with II.
860,
874
"'■"""
57 Auriga?
I
17 5 6
n
1 50
1 vF. vS. /E.
875
—
— —
I
21 42
I
o"7
1 vF. vS,
SiS
Dr. Herschel's Catalogue
in.
876 Dec. 2351 Piscium
877
1790.
Stars.
Feb. 23 2 6 Hy dree
May 6
24
878 Apr.
879
880
881
882
883
884
885
886
887
888
889
890
891
892
893
1792
894 Apr. 20
895
896
1793
2 14 (t) Ursas
73 Ursas
335 Ursae -
9 Ursae min
13(9/) Ursas min.
37 (£) Bootis
26 7 Serpentis
2719 (|) Coronas
28' 17 (<r) Coronas
20 (V) Coronas
25 Herculis
30
44 (vj) Herculis
22 (f) Bootis
J Feb. 4 34 (0) Gemin.
897
89«
899
900
901
902JMar.8
903lApr. 6
904I ~
}-
/
M.
18 Navis
4 Draconis
5 44
73 56
9 14
2 39
8 13
21 51
34 52
4 2 4 1
44 51
3 44
15 3 2
6 41
2 1
8 9n
3 4i
2 5
6 26
D. M.
n
1 43
o 22
12 29
!2 55
16 45
1 33
15 18
36 21
10 36 n
30 43 n
23 25] »
38
12
26*
o
g6
22
35
o 20
7
52
20
37
9
8
1 15
o 47
o 25
3i
17
Description.
vF.ph. iR.Jfa Sft whjch-is
partly involved in the ne-
bulosity.
vF. iR. r. <z'd. almost of equal
light throughout.
vF. ch. R. mbM, near $'d.
cF. S. iF.
eF. S.
z/F.S.
t>F, />L. R. 6M.
?F. t>S. ver. 300.
fF. v S. with 300 cL,
<?F. t>S. E. near par.
{Two nebulas, both eF. vS.
the p is the most n. dist.
2
<?F. z>S. R. with 300 ph.
vF. S. R. vglbM.
vF.pL.lE.lbM.
eF. vS. R. IbM.
eF.S.bM.
eF. vS. iF. ver. 300.
vF. vS.
vF. vS.
eF. S. vlbM.
9
32
10
24
Two nebulae. The most n.
andp.eF. S. The other
eF. vS. dist. 4'.
v F. S. nearly R. 6M.
Two nebulas just prece-
ding III. 703. Both eF.
vF. IE. r. 6M.
eF. S. iF. vlbU.
eF. vS. E. mer.
of goo new Nebulce, and Clusters of Stars,
5*7
in.
9°5
go6
9°7
908
9°9
9io
911
912
9*3
9H<
9*5
916
917
918
919
920
921
922
923
924
925
926
927
928
9*9
93°
93 1
932
1793-
Apr. 7
8
39 Ursas
942 Ursa?
May 5
Sept. 6
933
934
MDCCCII
1794
Apr. 1
Stars.
4 Draconis
6 Draconis
37 Ursas
Hydr.L.C.i 179
6 Hydras conti
64 Virginis
19 Bootis Hev.
1393 (0 Virgin.
53 Aquarii
Georgian planet
P
M. S.
37 3
12 31
16 26
23 36
39 i°
15 47
11 47
o 59
8 14
10 29
25 35
48 48
15 19
15 10
o 1
19 23
24 11
35 14
1
11
1
*3
25
2
18
5
o 20
26 17
9 25
27 19
12 23
8 .50
6"
16
11
I
D. M
8
8
35
10
35
19
5
27
14
2
3
39
44
47
2
1
22
11
5
27
10
17
44
5
35
18
19
11
o 58
Description.
¥b.
eF. vS. ver. 300.
v F. E. 2'/, i'6.
vF.F.npff. ii'Z,
<?F. z>S. iR. »/&M.
vF. vS. R.
z>F. />L. zF. r. some of the
stars visible.
vF. cL. zF.
?F. t>S. ver 300.
z>F. z>S.
vF. S. /E.
r>F.S.
<?F. vS. Stellar near a S/if.
r Two nebulae.
lBotht;F./>S. R./6M.
vF. vS. near a z>S/£.
eF. vS. E. near mer.
eF.pL. E.
i>F. z>S. 2z>S. stars in it.
vF.vS.R.lbM.
eF. S. r. ver. 300.
cF. S.
vF. S.fp.zcBft.
vF. S.
vF. S.
vF. S. E. mer.
^F. ver. 300.
eF. S. z'R.
eF. S. IE. fof a Sft.to which
it seems almost to be at-
tached, but is free from it.
The star is the 1st of 3,
making a S triangle.
vF. S. R. 6M.
vF. This nebula was seen
at 9 h 45', sidereal time, the
3X
51 8
Dr. Herschel's Catalogue
III.
1794.
Stars.
M.
s.
D. M. 5
r Description.
telescope being out of the
meridian.
935
Apr. 19
12 (£) Hydrae
crateris
/
15
11
w
401
. eF. S. bM.
936 Oct. 15
5 («) Cephei
/
7 54
»
16]
vF. er,
1797
937
Nov. 22
Neb. I. 274
/
25
3
«
53 3
vF. S. iR. bM.
93 8
Dec. 10
A double st*
P
9
5
n
lOl
eF.pL,. z'F.* See I. 273.
939
—
■ — —
f
4
I
35 ]
ieF. S.
94°
12
5 Dracon.Hev,
P
32
24
I
49 ]
1 vF. S. R. bM.
94i
—
— —
P
8
21
n
573
1 vF. pS. 2 S nf stars make a
a triangle with it.
94 s
—
. — —
f
4
16
n
59 1
1 tfF. E. near mer. ver. 300.
943
944
}-
5 (a) Urssemi.
f
46
2
1
281
f Two nebulae.
[Both z'F. z>S.r.dist. if par.
945
___
35 Draconis
P
47
10
I
1 17]
1 vF. S. E. n of a Sft.
94 6
20
4 (6) Ursae mi.
P
29
3i
n
1 57 ]
l z/F. vS. R.
947
—
— —
P
14 39
n
42-
t vF. cL. iF. vlbM.fofapB.
fi-
94 8
— .
— _
f
2
20
n
1 3
l eF. vS. E. near mer.
949
___
, — —
f
14 44
n
2 29
1 eF. S. IE. near par.
95o
I
24
18
n
1 13.
t z'F. S. r. It is preceded by a
S. patch ofjt which ap-
pears almost like this ne-
bula, but more resolved.
95i
—
4 Cephei of
Bode's Cat.
P
21
18
I
1 25
1 eF. S. better with 320.
1798
lDec.9
fTvvo nebulae within 1' of
95%
953
2 (7/) Ononis
P
10
20
I
1 34
1 \ each other; mer. Both
I fF. vS.
954
10
8 Ceti -
J
^7
5
f
j
1 15
1 eF. S.
955
—
21 Ceti
P
3
46
n
4
1 cF. vS. iR.
95 ( >
1799
18 (e) Eridani
P
15
21
J
53
1 vF. vS. 2 or 3' n of 2SJL
957
958
1 June
J 2 9
93 Herculis
P
4
3
3
59
n
1 33
1 37
(Two nebulas.
1 I Both z'F. vS.
mios.Tra7u-MDCCC T I.Fla£eXV I.p. 518.
J(Z&„3.
3%ck£.
*3fy'a„'7.
P
v" f' mm ' ' 1 -% /
4 — - — ■ — ■ — .* ■■ — -<...„„ ,1/. /
n - Vs ' ' //T 1
^/Za-„8
of 500 new Nebula?, and Clusters of Stars.
519
in.
959
960
961
962
963
9 6 5
9 66
967
968
9 6 9
97o
97i
972
973
974
975
976
1799.
Dec. 19
1801
Apr. 2
}-
Nov. 28
Dec. 6
1802
J Jan. 1
May 21
Stars.
16 Eridani
19 Eridani
2o8(N)Caraelop.
of Bode's Cat.
50 (a) Ursa?
16 (£) Ursas mi,
22 (s) Ursas mi
977 Sep. 26
978
2 (??) Coronas
186 P. Camelop.
of Bode's Cat,
P
P
P
P
P
P
P
P
P
I
M. S.
6 37
1 19
2 43
20 51
157 S 6
119 54
117 22
118 o
72 10
37 3 1
24 19
20 34
5 7
14 15
10 49
26 50
9 49
33 19
D. M
O 26
n
n
f
13
4 6>
15
16
5
56
29
l 52
39
28
3 1
10
8
o 37
o 2
1 S3
o 5«
Description.
The 2d of 2 vF. vS. 1%'ffl.
60.
vF. vS. ver. 300.
vF. vS.
vF. vS.Jp. zpBft.
eF. S, z'F.
cF. S. Stellar, ver. 300. just
p. a S/t.
vF.vS.
vF. vS.
Two nebulas. The 1st vF.
S.
The 2d nf. the 1st *F. vS.
eF. S.
vF.ph. r.
eF. vS. R.
vF. v$. R. 6M.
t;F. S. IE, mer. r.
Two nebulas ; the preced-
ing cF. S. 6M. the foil.
-< vF. vS. it follows the 1st
a few seconds, and is 3'
more north.
eF. S. iF.
eF. vS. 300 confir.
eF.pL. vlbM. just « of %/£.
3 x *
52 o
Dr. Herschel's Catalogue
Fourth Class. Planetary Nebula.
Stars with Burs, with milky Chevelures, with short Rays, remarkable Shapes, &c.
IV.
59 Mar. 23 55 Ursas -
60
61
6z
63
64
65
1789.
Stars.
Apr. 1 236 Ursas
14
64 (y) Ursae
24|6g Ursa? Hev.
1790
Mar. 4
6 Navis
28 Monocerotis
/
/
/
/
/
P
M.
4 5i
8 $7
3 56
2 27
1 24
7 4 1
5 1 49
72
/
/
»
o 19
1 25
/
/
n
D. M.
o 23
2 28
1 33
1 2
o 26
Description.
dB.S.R.BN. The N is con-
siderably well defined, and
the chevelure vF.
vB. R. Planetary, but very
ill defined. The indis-
tinctness on the edges is
sufficiently extensive to
make this a step between
planetary neb. and those
which are described
vfmbM.
cB. BrN with z>FE branches
about 30 np ff. 7 or 8'/,
4 or 5'b.
cB. quite R. A large place in
the middle is nearly of an
equal brightness. To-
wards the margin it is less
bright.
cB. cL. iR. er. vgmbM. 4'
diam. I suppose, with a
higher power, I might
have seen the stars.
A beautiful planetary nebu-
la, of a considerable de-
gree of brightness; not
very well defined, about
12 or 15" diam.
A pretty considerable star,
9 or 10m. visibly affect-
ed with vF. nebulosity,
of very little extent all
of 500 new Nebula, and Clusters of Stars.
521
IV.
1790.
Stars,
66'
Mar. 18
67
68
69 Nov. 30
17 Ursae -
66 Ursas -
1945 Lyncis
i
26 Auriga
Hevelii
or 31
P
P
u,
16 29
° 39
4 15
88 24
24 59
D. M.
/
n
3 6
1 55
44
11
26
Description.
around. A power of 300
shewed the same, but gave
a little more extent to the
nebulosity. The2sd Mon-
cerotis was quite free from
nebulosity.
A small star with apB. fan-
shaped nebula. The star
is on the p side of the di-
verging chevelure, and
seems to be connected
with it.
pB. ph. R. The greatest
part of it equally B, then
fading away p suddenly ;
between 2 and 3' diam.
vB. S. exactly R. BNM.and
t;F. chev. vg. joining to
the N. In a lower situa-
tion the chev. might not
be visible, and this neb.
would then appear like an
ill defined planetary one.
A most singular phenome-
non; Aft 8m. with a faint
luminous atmosphere of a
circular form, about 3' in
diam. The star is perfect-
ly in the centre, and the
atmosphere is so diluted,
faint, and equal through-
out, that there can be no
surmise of its consisting of
stars, nor can there be a
doubt of the evident con-
nection between the at-
mosphere and the star,
Dr. Herschel's Catalogue
IV.
70
71
72
73
1790.
Stars.
1791
Mar. 6
May 24
1792
Sep. 15
1793
Sep. 6
6 Draconis
87 (I) Bootis
34,Cygni -
16 (O Cygni
/
/
P
f
M. S.
50 27
16 5
10
2 51
/
?z
/
D. M
o 27
o 44
o
23
Description.
Another star, not much
less in brightness, and in
the same field with the
above, was perfectly free
from any such appear-
ance.
cB. R. almost equally B
throughout, resembling a
very ill defined planetary
neb. about i'diam.
star 7.6m. enveloped in
extensive milky nebulo-
sity. Another star 7m. is
perfectly free from such
appearance.
A double star of the 8th
magnitude, with a faint
south - preceding milky
ray joining to it, 8'/, and
ii' broad.
A bright point, a little ex-
tended, like two points
close to one another ; as
bright as a star of the 8.9
magnitude, surrounded by
a very bright milky nebu-
losity suddenly termina-
ted, havingtheappearance
of a planetary nebula with
a lucid centre; the border
however is not very well
defined. It is perfectly
round,and I suppose about
half a minute in diam. It
of 500 new Nebula, and Clusters of Stars.
523
IV.
*793-
1794
74 Oct. 18
75
76 Sep
1798
it. 9
77
Dec. 19
Stars.
7 Cephei -
7 Cephei
3 (*?) Cephei
16 Eridani
/
/
M. S.
24 57
14 40
10 31
4 56
n
/
/
ft
M. D.
1 22
46
1 36
o 14
Description.
is of a middle species, be-
tween the planetary ne-
bulae and nebulous stars,
and is a beautiful pheno-
menon.
A star 7m. very much af-
fected with nebulosity,
which more than fills the
field. It seems to extend
to at least a degree all
around ; smaller stars,
such as 9 or 1 om . of which
there are many, are per-
fectly free from this ap-
: pearance.
A star 7.8m. is perfectly
free from this appearance.
Three stars about 9m. in-
volved in nebulosity. The
whole takes up a space of
about i^'diam. other stars
of the same size are free
from nebulosity.
cF. vL. iF. a sort of $NM.
The nebulosity 6 or 7'.
The N seems to consist
of stars, the nebulosity is
of the milky kind. It is a
pretty object.
A star about 9 or 10m. with
a nebulous ray to the
south-precedingside. The
ray is about 1 J-' long. The
star may not be connected
with it.
524
Dr. Herschel's Catalogue
IV.
1801.
Stars.
78 Nov. 8
8 Urseemin. of
Bode's Cat.
P
M. S.
25 o
n
D. M.
O 12
Description.
['
cB. R. about if diarn.
Somewhat approaching
to a planetary nebula,
with a strong hazy border.
Fifth Class. Very large Nebula.
v,
45
4 6
1789.
Apr. 12
1790
47 April i
48
49
50
51
i74,8(/3)Ursa3
Oct. g
1798
Mar. 4
April 6
Stars.
64 (7) Ursas -
30 (tp) Ursa?
< Fornacis L. C.
182 - -
Dec. 2841 Persei Hev.
e Pixidis Na. L.
C. 831 -
4 Draconis -
/
/
/
/
/
M. S.
O 9
IO 4
10 9
8 7
22 o
35 s6
14 48
/
M. D.
1 23
41
1 39
O 2
o i,5
o 43
o 20
Description.
cB. £F. E. mer. LBN. with
F. branches 7 or 8'/, 5 or
6'b.
vB, wE. r. io'/, 2'6. There
is an unconnected pretty
bright star in the middle.
vB. i»E. np ff. vgmbM. 8'/,
a'6.
»B. E. 75 # //. 8' long. A
very bright nucleus, con-
fined to a small part, or
about 1' diam.
6 or 7 small stars, with faint
nebulosity between them,
of considerable extent,
and of an irregular figure.
vF. vS. IE. xgfpnf. IbWL.
8'1, 5 or 6'b.
vF. mE. yd" npff. About
25'/, and losing itself im-
perceptibly, about 6 or 7'
broad.
of 500 new Nebula, and Clusters of Stars.
fty f
V.
1801.
Stars.
M. S.
D. M.
Description.
52
Nov.28
50 (a) Ursse
p
l 7 49
ra
1 30
]
cB. E. mer. r/g-fcM. About
5'/. and 3' broad ; the ne-
bulosity seems to be of*
the milky kind; it loses
itself imperceptibly all a-
round. The whole breadth
of the sweep seems to be
affected with very faint
nebulosity.
Sixth Class. Very compressed and rich Clusters of Stars.
Additional Tel. Cluster, com. compressed,
Abbreviations.] sc. scattered, co. coarsely.
VI.
1790.
$6 Mar. 4
37 Feb
38
89
179*
23
Aug.25
*793
Mar. 3
Star s
6 Navis
26 Hydras -
50 (y) Aquilaa
£ Pixidis Naut.
L. C. 777 -
M. S.
P
P
MDCCCII.
8 45
79 So
14 50
20 39
/
n
1
I
D. M.
1 55
1 18
o 10.
Description.
A t>. com. cl. of S, and some
1ft. E near mer. The
most compressed part is
about 87, and 2'6. with
many scattered to a con-
siderable distance.
A v. com. and very rich cl.
of stars. The stars are of
2 sizes, some considerably
L. and the rest next to
invisible. The com. part
5 or 6' in diam.
6-B. S. z'F. er. Some of theft.
are visible.
A cl. of lft. considerably
rich z'R. above 15' diam.
3Y
X26
Dr. Herschel's Catalogue
VI.
40
41
42
J 793-
May 12
1-797
Dec. 1 2
53 (1/) Serpentis
1798
Sep. 9
Stars.
35 Draconis -
3 (,) Cephei
P
P
M. S.
48 17
22 6
13 26
»
y
/
D. M,
O 2
1 7
i 6
Description.
A very beautiful e com. cl.
of JL extremely rich, 5 or
6' in diam. gradually more
compressed towards the
centre.
R. r. about 3' diam. tg-6M.
I suppose it to be a clus-
ter of stars extremely
compressed. 300 confirms
the supposition, and shews
a few of the stars ; it must
be immensely rich.
A beautiful compressed cl.
of Sft. extr. rich, of an
i F. The preceding part of
it is round, and branching
out on the following side,
both towards the n. and
towards the /. 8 or 9' in
diam.
Seventh Class. Pretty much
compressed Clusters of large or small Stars.
VII.
1788.
Stars.
M. S.
D. M.lS
1
Description.
56
Dec. 16
11 (jQ) Cassiop
P
9 57
n
2 6
1
A p. com. cl. of Sft. of se-
veral sizes, cons. rich. E.
57
59
3 1
1790
Mar. 4
Sept. 11
40 Auriga? -
6 Navis
18 ($) Cygni
f
f
f
8 28
5 18
1.8 38
n
f
J
1 25
29
1
1
1
near par. 5 or 67.
A compressed cl. of vS stars
z'F. 6' diam. consid. rich.
A p. com. and rich cl. of S
stars zR. 7 or 8' diam.
A v. rich cl. of Lft. conside-
rably compressed, above
of goo new Nebula, and Clusters of Stars.
527
VII.
60 Dec. 28
61
62
6$
64,
65
Aug. 21
67 J
1790.
1793
Mar,
8
66 Oct. 18
1799
lan. 30
Stars.
47 (x) Persei
41 Persei Hev.
19 Aquilae -
3C
Pixidis Naut,
L. C. 777 -
2 Navis
7 Cephei -
15 (V) Canis
/
/
M.
3 3°
3 8
o 26
2 25
20 55
16 10
16 45
42 33
D. M
o 50
56
1 24
24
1 9
38
1 7
o 14
Description.
15' diam. by the size of
theft, it is situated in the
milky-way, towards us.
AL. cl. oicLft.p. com. and
very rich. z'R. 7' diam.
A beautiful cl. of hft. v rich,
and considerably com.
about 15' diam.
A S. p. com. cl. of stars not
very rich.
A L. cl. of scattered Sft. zF.
considerably rich.
A L. cl. of ft. of a middling
size, i E. considerably
rich. The stars are chiefly
in rows.
A S. cl. of vS ft. considera-
bly rich and compressed.
A cl. of cons. com. vS and
L. stars about 12' diam.
considerably rich.
A cl. of com. stars, consi-
derably rich.
sYs
A3 8
Dr. Herschel's Catalogue, &c.
Eighth Class. Coarsely scattered Clusters of Stars.
VIII
79
80
82
83
84
«5
Dec. 16
18
*7 8 9
July 18
1790
Sept. 11
QO
Dec. 28
Stars.
11 (|G) Cassiop
1 Camelopar.
5 Vulpeculee
57 c yg ni -
51 Cygni -
33 («) Persei
4,1 Persei Hev.
1792
86 Sept. 15 34 Cy
87
88
1793
Mar. 8
1799
Dec. 28
gni
2 Navis
46 (|) Persei
/
M. S.
SO 3,5
4* 3 6
2 46
1 o
25 24
9 14
2 42
9 43
7 10
27 *3
D. M.
W
/
n
1 5
1 29
a 4
o 52
o 1
1 36
O 2
o 151
15
1 29
Description.
A coarsely sc. cl. of hft.
mixed with smaller ones,
not very rich.
A cl. of S. stars, containing
one large one, 10; 9m. 2;
or 3' diam. not rich.
A sc. cl. of chft. i¥. pretty
rich, above 15' in extent.
A L. cl. of fiS. stars of se-
veral sizes.
A cl. of sc. stars, above 15'
diam. pretty rich, joining
to the milky-way, or a
projecting part of it.
A cl. of Sft. not very rich.
A coarsely sc. cl. of hft.
pretty rich.
A coarsely sc. cl. ofL stars,,
of a right-angled triangu-
lar shape.
A small cl. of S. stars, not
very rich.
A cl. of coarsely sc. hft,
about 15' diam.
JPhilos Jmn s M T>CCCJ U J late WR.p.BiS .
■ -y^jy^o .
M.
T xa,^2.
w
, /fBft.vire